JPS621273A - Reverse-conducting gto thyristor - Google Patents

Reverse-conducting gto thyristor

Info

Publication number
JPS621273A
JPS621273A JP13993185A JP13993185A JPS621273A JP S621273 A JPS621273 A JP S621273A JP 13993185 A JP13993185 A JP 13993185A JP 13993185 A JP13993185 A JP 13993185A JP S621273 A JPS621273 A JP S621273A
Authority
JP
Japan
Prior art keywords
layer
diode
thyristor
section
contact
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP13993185A
Other languages
Japanese (ja)
Inventor
Osamu Hashimoto
理 橋本
Yoshikazu Takahashi
良和 高橋
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP13993185A priority Critical patent/JPS621273A/en
Publication of JPS621273A publication Critical patent/JPS621273A/en
Pending legal-status Critical Current

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  • Thyristors (AREA)

Abstract

PURPOSE:To compound a diode having small forward voltage adjacently into one semiconductor substrate, and to ensure even reverse with-standing voltage between a gate and a cathode by thinning the diode section for a reverse- conducting GTO thyristor while forming the same conduction type high impurity concentration layer to the surface of a thinned layer. CONSTITUTION:A p-layer 22 for a diode section is made thinner than a p-base layer 13 for a GTO thyristor section through etching, etc. A p<+> layer 5 is shaped onto the surface of the p-layer 22, and functions as the stoppage of the extension of a depletion layer. A diode anode electrode 9 being in contact with the p<+> layer 5, thyristor cathode electrodes 7 being in contact with an n-emitter layer 14, gate electrodes 8 being in contact with the p base layer 13 and a thyristor anode electrode 6 serving as a diode cathode electrode being in contact with a p-emitter layer 11 are formed severally, and an electrode body 10 with a stepped section is pressure-welded to the thyristor cathode electrodes 7 and the diode anode electrode 9. A resistor 20 is shaped, thus ensuring withstanding voltage between a gate and a cathode for the thyristor without scaling up an isolation region 3.

Description

【発明の詳細な説明】[Detailed description of the invention] 【発明の属する技術分野】[Technical field to which the invention pertains]

本発明は、同一半導体基板内にGTOサイリスタとそれ
に逆並列のダイオードを設けた複合素子としての逆導通
GTOサイリスタに関する。
The present invention relates to a reverse conducting GTO thyristor as a composite element in which a GTO thyristor and a diode antiparallel to the GTO thyristor are provided in the same semiconductor substrate.

【従来技術とその問題点】[Prior art and its problems]

第2図に示すようなGTOインバータにおいて、逆並列
に接続されているGTOサイリスタ31とダイオード3
2を一体化して回路構成を簡単にすることが行われてい
る。このような逆導通GTOサイリスタにおいては可制
御電流が大きく、ダイオード部の逆回復時間が短く、か
つ大電流をターンオフするためにゲート、カソード間の
耐圧が高くなければならない、またGTOサイリスタの
順方向耐圧が高いことが必要である。
In a GTO inverter as shown in Fig. 2, a GTO thyristor 31 and a diode 3 are connected in antiparallel.
2 are integrated to simplify the circuit configuration. In such a reverse conduction GTO thyristor, the controllable current is large, the reverse recovery time of the diode part is short, and the withstand voltage between the gate and cathode must be high in order to turn off the large current. It is necessary to have high pressure resistance.

【発明の目的】[Purpose of the invention]

本発明は、上記の諸条件を満足する逆導通GTOサイリ
スタ、すなわち可制御電流が大きく、ダイオード部の逆
回復時間が短く、ゲート、カソード間の耐圧が高く、サ
イリスク順方向耐圧が高い逆導通GTOサイリスタを提
供することを目的とする。
The present invention is a reverse-conducting GTO thyristor that satisfies the above conditions, that is, a reverse-conducting GTO thyristor with a large controllable current, a short reverse recovery time of the diode part, a high breakdown voltage between the gate and the cathode, and a high thyristor forward breakdown voltage. The purpose is to provide thyristors.

【発明の要点】[Key points of the invention]

本発明は、pnpn4層からなり第一導電形のベース層
に接触するゲート電極が設けられたGTOサイリスタ部
と、そのベース層と隣接する第二導電形のベース層との
間のpn接合の延長面を挟む912層からなるダイオー
ド部を同一半導体基板内に有する透導11GToサイリ
スタの、ダイオード部の第一導電形の層がそれにつづく
 GTOサイリスタ部の第一導電形のベース層より薄く
、かつその表面により高濃度の第一導電形の層を介して
接触する電極がGTOサイリスタ部の第二導電形のエミ
ッタ層に接触する主電極に接続されていることにより上
記目的を達成する。
The present invention provides an extension of a pn junction between a GTO thyristor part made of four pnpn layers and provided with a gate electrode in contact with a base layer of a first conductivity type, and a base layer of a second conductivity type adjacent to the base layer. A layer of the first conductivity type of the diode part of a transparent 11GTo thyristor having a diode part consisting of 912 layers sandwiching surfaces in the same semiconductor substrate is thinner than the base layer of the first conductivity type of the GTO thyristor part, and is thinner than the base layer of the first conductivity type of the GTO thyristor part. The above object is achieved by connecting the electrode which is in contact with the first conductivity type layer with a higher concentration at the surface to the main electrode which is in contact with the second conductivity type emitter layer of the GTO thyristor section.

【発明の実施例】[Embodiments of the invention]

第1図は本発明の一実施例を示し、シリコン基板にはG
TOサイリスタ部l、ダイオード部2および分離領域3
が形成されている。GTOサイリスタ部lはpエミッタ
11111.nベース層12.pヘ−ス層13.  n
エミッタ層14からなり、ダイオード部2は0層21.
 9層22からなり、側面18はベベル成形され、ダイ
オード部のpn接合とGTOサイリスタ部のp+nベー
ス層間のJ8接合とは連続している。nベース層12お
よび0層21のこのpn接合より遠い側にはりん拡散な
どによりn′″層4が形成され、実質的にpin構造と
する既知の技術が使用されている。ダイオード部の9層
22はGToサイリスタ部のpベース層13よりエツチ
ング等によって薄くされている。p122を薄くするこ
とにより、ダイオード部に導入されるライフタイムキラ
ーの量を多くしてもダイオードの順電圧V。 を過大にすることがないので、ダイオード部のライフタ
イムを短くでき、逆回復時間の短い高速度ダイオードと
することができる。しかしGTOサイリスタ部1の順方
向、すなわちダイオード部2の逆方向の電圧を印加した
とき、ダイオード部の9層22に広がる空乏層がGTO
サイリスタ部のカソード電極と等電位のダイオード部の
アノード電極に達するのを防ぐため、9層22の表面に
はほう素拡散などによりp゛層5形成され、空乏層の広
がりを止める働きをする。この結果この逆導通GTOサ
イリスタの順方向耐圧の確保が容易である。この99層
5に接触するダイオードアノード電極9.nエミッタ層
14に接触するサイリスタカソード電極1.  pベー
ス層13に接触するゲート電$1+8.  pエミッタ
層11に接触するダイオードカソード電極を兼ねるサイ
リスク7ノード電掻6がそれぞれ設けられ、サイリスタ
カソード電極7とダイオードアノード電?!i9に、段
差を有する電極体10が圧接される。GTOサイリスタ
部1において、ゲート電WIBとカソード電極7の間に
逆電圧をかけてターンオフさせる場合、ゲート電極8と
同じpWAに接触するダイオードアノード電極9とサイ
リスタカソード電極7との間が高抵抗でなければ電圧は
かからない、しかるに本発明により両者の間に段差があ
り、抵抗20が形成されるので、分離領域3を大きくす
ることなくサイリスクのゲート。 カソード間の耐圧が確保される。 今、第1図に記入したようにダイオード部のpn接合に
連続しているGTOサイリスク部のJ震接合からnエミ
ッタ層14の表面までの高さをH5この表面とダイオー
ド部のp゛層5表面までの段差をhとした場合、hも大
きくとればダイオード部2の2層側の厚さが薄くなり、
上述のようにライフタイムを短(しても順電圧を抑える
ことができるためダイオード部の高速化が達成でき、ま
た分離領域3の抵抗20も大き(なってGTOサイリス
タ部1のゲート、カソード間に十分な逆電圧が印加でき
、同時にターンオフ時のダイオード部2からの電流のし
み出しも減少し、GTOサイリスタの可制御電流が大き
くなる。しかしhを大きくしすぎると順方向耐圧が小さ
くなる。 第3図は厚さt、が45Onのシリコン基板で、pエミ
ッタ層の高さHが100#111+分離部3の幅Wが約
1鮪の逆導通GTOサイリスタのhと順方向耐圧、可制
御電流との関係を示す、この結果から60μ≦h≦75
β1、すなわちダイオード部の厚さが375〜390μ
のときが望ましいことがわかり、2000Aの可制御電
流と2500 Vの耐圧が得られた。 【発明の効果] 本発明によれば、逆導通GTOサイリ″スタのダイオー
ド部の厚さを薄くすると共に薄くされた層の表面に空乏
層の広がりを阻止する同導電形の高不純物濃度層を設け
ることにより、可制御電流の大きなGTOサイリスタと
高速ではあるが順電圧の大きくないダイオードを一つの
半導体基板内に近接して複合化でき、かつGTOサイリ
スタのターンオフ過程に必要不可欠のゲート、カソード
間道耐圧をも確保できるので得られる効果は極めて大き
い。
FIG. 1 shows an embodiment of the present invention, in which a silicon substrate has a G
TO thyristor section 1, diode section 2 and isolation region 3
is formed. GTO thyristor section l has p emitter 11111. n base layer 12. p-hose layer 13. n
The diode section 2 consists of an emitter layer 14 and an 0 layer 21.
It consists of nine layers 22, the side surface 18 is bevel-shaped, and the pn junction of the diode part and the J8 junction between the p+n base layers of the GTO thyristor part are continuous. On the side of the n base layer 12 and the 0 layer 21 far from this pn junction, an n'' layer 4 is formed by phosphorus diffusion or the like, using a known technique to create a substantially pin structure. The layer 22 is made thinner than the p base layer 13 of the GTo thyristor section by etching etc. By making p122 thinner, the forward voltage V of the diode can be maintained even if the amount of lifetime killer introduced into the diode section is increased. Since the voltage is not increased excessively, the lifetime of the diode section can be shortened, and a high-speed diode with a short reverse recovery time can be achieved. When the voltage is applied, the depletion layer that spreads in the 9th layer 22 of the diode part
In order to prevent the depletion layer from reaching the anode electrode of the diode section, which has the same potential as the cathode electrode of the thyristor section, a p layer 5 is formed on the surface of the nine layer 22 by boron diffusion, etc., and serves to stop the spread of the depletion layer. As a result, it is easy to ensure the forward breakdown voltage of this reverse conducting GTO thyristor. Diode anode electrode 9 in contact with this 99 layer 5. Thyristor cathode electrode 1 in contact with n emitter layer 14. Gate voltage $1+8. in contact with p base layer 13. A thyristor 7-node electrode 6 which also serves as a diode cathode electrode in contact with the p emitter layer 11 is provided, and the thyristor cathode electrode 7 and the diode anode electrode 6 are connected to each other. ! The electrode body 10 having a step is pressed into contact with i9. In the GTO thyristor section 1, when a reverse voltage is applied between the gate electrode WIB and the cathode electrode 7 to turn it off, there is a high resistance between the diode anode electrode 9 and the thyristor cathode electrode 7, which are in contact with the same pWA as the gate electrode 8. However, according to the present invention, there is a step between the two and a resistor 20 is formed, so that the isolation region 3 can be removed without increasing the size of the gate. Withstand voltage between cathodes is ensured. Now, as indicated in Fig. 1, the height from the J-junction of the GTO silisk section that is continuous to the p-n junction of the diode section to the surface of the n emitter layer 14 is H5. If the step to the surface is h, if h is also made larger, the thickness of the second layer side of the diode part 2 will be thinner,
As mentioned above, even if the lifetime is shortened (the forward voltage can be suppressed, the speed of the diode section can be increased), and the resistance 20 of the isolation region 3 is also large (as a result, the resistance between the gate and cathode of the GTO thyristor section 1 is A sufficient reverse voltage can be applied to , and at the same time, current seepage from the diode section 2 during turn-off is reduced, increasing the controllable current of the GTO thyristor. However, if h is made too large, the forward breakdown voltage becomes small. Figure 3 shows a silicon substrate with a thickness t of 45 On, a reverse conduction GTO thyristor with a p emitter layer height H of 100#111 + width W of the isolation part 3 of about 1 inch, and forward breakdown voltage and controllable h. From this result, which shows the relationship with the current, 60μ≦h≦75
β1, that is, the thickness of the diode part is 375 to 390μ
It was found that a controllable current of 2000 A and a breakdown voltage of 2500 V were obtained. [Effects of the Invention] According to the present invention, the thickness of the diode portion of a reverse conduction GTO thyristor is reduced, and a highly impurity concentration layer of the same conductivity type is formed on the surface of the thinned layer to prevent the spread of a depletion layer. By providing a GTO thyristor with a large controllable current and a high-speed diode with a low forward voltage, it is possible to combine them in close proximity in one semiconductor substrate. The effect obtained is extremely large because it can also ensure road pressure resistance.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例の要部断面図、第2図はGT
Oインバータの回路図、第3図は本発明により形成され
る段差の大きさhと逆導通GTOサイリスタの順方向耐
圧、可制御電流との関係線図である。 1:GTOサイリスタ部、2:ダイオード部、3:分離
領域、7:カソード電極、8:ゲート電極、9:ダイオ
ードアノード電極、10:電極体、h:段差。 第1図 第2図
Fig. 1 is a sectional view of essential parts of an embodiment of the present invention, Fig. 2 is a GT
The circuit diagram of the O inverter, FIG. 3, is a diagram showing the relationship between the size h of the step formed by the present invention, the forward breakdown voltage, and the controllable current of the reverse conduction GTO thyristor. 1: GTO thyristor section, 2: diode section, 3: separation region, 7: cathode electrode, 8: gate electrode, 9: diode anode electrode, 10: electrode body, h: step. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 1)交互に異なる導電形を有して隣接する4層からなり
第一導電形のベース層に接触するゲート電極が設けられ
たGTOサイリスタ部と、該ベース層と隣接する第二導
電形のベース層との間のpn接合の延長面を挟む異なる
導電形の2層からなるダイオード部を同一半導体基板内
に有するものにおいて、ダイオード部の第一導電形の層
がそれにつづくGTOサイリスタ部の第一導電形のベー
ス層より薄く、かつその表面により高濃度の第一導電形
の層を介して接触する電極がGTOサイリスタ部の第二
導電形のエミッタ層に接触する主電極に接続されたこと
を特徴とする逆導通GTOサイリスタ。
1) A GTO thyristor section consisting of four adjacent layers having alternately different conductivity types and provided with a gate electrode in contact with a base layer of a first conductivity type, and a base of a second conductivity type adjacent to the base layer. In a semiconductor substrate having a diode section consisting of two layers of different conductivity types sandwiching an extension surface of a pn junction between the two layers, the first conductivity type layer of the diode section is the first conductivity type layer of the GTO thyristor section following it. The electrode that is in contact with the first conductivity type layer, which is thinner than the base layer of the conductivity type and has a higher concentration on its surface, is connected to the main electrode that is in contact with the emitter layer of the second conductivity type of the GTO thyristor section. Features reverse conduction GTO thyristor.
JP13993185A 1985-06-26 1985-06-26 Reverse-conducting gto thyristor Pending JPS621273A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13993185A JPS621273A (en) 1985-06-26 1985-06-26 Reverse-conducting gto thyristor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13993185A JPS621273A (en) 1985-06-26 1985-06-26 Reverse-conducting gto thyristor

Publications (1)

Publication Number Publication Date
JPS621273A true JPS621273A (en) 1987-01-07

Family

ID=15256999

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13993185A Pending JPS621273A (en) 1985-06-26 1985-06-26 Reverse-conducting gto thyristor

Country Status (1)

Country Link
JP (1) JPS621273A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0923136A2 (en) * 1997-10-24 1999-06-16 Asea Brown Boveri AG Gate turn off thyristor with stop layer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0923136A2 (en) * 1997-10-24 1999-06-16 Asea Brown Boveri AG Gate turn off thyristor with stop layer
EP0923136A3 (en) * 1997-10-24 1999-12-22 Asea Brown Boveri AG Gate turn off thyristor with stop layer
US6107651A (en) * 1997-10-24 2000-08-22 Asea Brown Boveri Ag Gate turn-off thyristor with stop layer

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